Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
| # | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 57008 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{4}M_{7}$ | 0.6139 | 0.7848 | 0.7822 | [M:[1.0, 0.875, 0.6719, 1.0625, 0.7344, 1.3281, 0.9375], q:[0.7656, 0.2344], qb:[0.5625, 0.5625], phi:[0.4688]] | [M:[[0], [-8], [-5], [4], [-1], [5], [-4]], q:[[1], [-1]], qb:[[4], [4]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{6}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{7}$, ${ }M_{1}\phi_{1}^{2}$ | ${}$ | -4 | t^2.203 + 2*t^2.391 + t^2.625 + 2*t^2.813 + t^3. + t^3.797 + 2*t^3.984 + t^4.406 + 2*t^4.594 + 6*t^4.781 + t^4.828 + 2*t^5.016 + 5*t^5.203 + t^5.25 + 2*t^5.391 + 2*t^5.438 + 4*t^5.625 + t^5.813 - 4*t^6. + 3*t^6.187 + 3*t^6.375 - t^6.422 + 3*t^6.609 + 3*t^6.797 + 4*t^6.984 + t^7.031 + 8*t^7.172 + 2*t^7.219 + 3*t^7.406 + t^7.453 + 10*t^7.594 + 2*t^7.641 + 4*t^7.781 + 4*t^7.828 + t^7.875 + 7*t^8.016 + 2*t^8.063 - 2*t^8.203 + 4*t^8.25 - 9*t^8.391 + 5*t^8.438 + 3*t^8.578 - 2*t^8.625 + 8*t^8.766 - 9*t^8.813 - t^4.406/y - t^6.609/y - t^7.031/y - t^7.219/y + (3*t^7.594)/y + (2*t^7.781)/y + t^7.828/y + (4*t^8.016)/y + (6*t^8.203)/y + (2*t^8.391)/y + (2*t^8.438)/y + (2*t^8.625)/y + t^8.813/y - t^4.406*y - t^6.609*y - t^7.031*y - t^7.219*y + 3*t^7.594*y + 2*t^7.781*y + t^7.828*y + 4*t^8.016*y + 6*t^8.203*y + 2*t^8.391*y + 2*t^8.438*y + 2*t^8.625*y + t^8.813*y | t^2.203/g1 + 2*g1^3*t^2.391 + t^2.625/g1^8 + (2*t^2.813)/g1^4 + t^3. + g1*t^3.797 + 2*g1^5*t^3.984 + t^4.406/g1^2 + 2*g1^2*t^4.594 + 6*g1^6*t^4.781 + t^4.828/g1^9 + (2*t^5.016)/g1^5 + (5*t^5.203)/g1 + t^5.25/g1^16 + 2*g1^3*t^5.391 + (2*t^5.438)/g1^12 + (4*t^5.625)/g1^8 + t^5.813/g1^4 - 4*t^6. + 3*g1^4*t^6.187 + 3*g1^8*t^6.375 - t^6.422/g1^7 + (3*t^6.609)/g1^3 + 3*g1*t^6.797 + 4*g1^5*t^6.984 + t^7.031/g1^10 + 8*g1^9*t^7.172 + (2*t^7.219)/g1^6 + (3*t^7.406)/g1^2 + t^7.453/g1^17 + 10*g1^2*t^7.594 + (2*t^7.641)/g1^13 + 4*g1^6*t^7.781 + (4*t^7.828)/g1^9 + t^7.875/g1^24 + (7*t^8.016)/g1^5 + (2*t^8.063)/g1^20 - (2*t^8.203)/g1 + (4*t^8.25)/g1^16 - 9*g1^3*t^8.391 + (5*t^8.438)/g1^12 + 3*g1^7*t^8.578 - (2*t^8.625)/g1^8 + 8*g1^11*t^8.766 - (9*t^8.813)/g1^4 - t^4.406/(g1^2*y) - t^6.609/(g1^3*y) - t^7.031/(g1^10*y) - t^7.219/(g1^6*y) + (3*g1^2*t^7.594)/y + (2*g1^6*t^7.781)/y + t^7.828/(g1^9*y) + (4*t^8.016)/(g1^5*y) + (6*t^8.203)/(g1*y) + (2*g1^3*t^8.391)/y + (2*t^8.438)/(g1^12*y) + (2*t^8.625)/(g1^8*y) + t^8.813/(g1^4*y) - (t^4.406*y)/g1^2 - (t^6.609*y)/g1^3 - (t^7.031*y)/g1^10 - (t^7.219*y)/g1^6 + 3*g1^2*t^7.594*y + 2*g1^6*t^7.781*y + (t^7.828*y)/g1^9 + (4*t^8.016*y)/g1^5 + (6*t^8.203*y)/g1 + 2*g1^3*t^8.391*y + (2*t^8.438*y)/g1^12 + (2*t^8.625*y)/g1^8 + (t^8.813*y)/g1^4 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
| # | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
| id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
|---|
Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 55437 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{6}$ | 0.609 | 0.7775 | 0.7832 | [M:[1.0, 0.9148, 0.6967, 1.0426, 0.7393, 1.3033], q:[0.7607, 0.2393], qb:[0.5426, 0.5426], phi:[0.4787]] | t^2.218 + 2*t^2.346 + t^2.744 + t^2.872 + t^3. + t^3.128 + t^3.782 + 2*t^3.91 + t^4.436 + 2*t^4.564 + 6*t^4.692 + t^4.962 + t^5.09 + 3*t^5.218 + 3*t^5.346 + 2*t^5.474 + t^5.489 + t^5.617 + 2*t^5.744 + t^5.872 - 3*t^6. - t^4.436/y - t^4.436*y | detail |